EP1146732A1 - Photosignal-Spannungswandlerschaltung in Bildsensoren mit entfernten Integratoren - Google Patents
Photosignal-Spannungswandlerschaltung in Bildsensoren mit entfernten Integratoren Download PDFInfo
- Publication number
- EP1146732A1 EP1146732A1 EP01400894A EP01400894A EP1146732A1 EP 1146732 A1 EP1146732 A1 EP 1146732A1 EP 01400894 A EP01400894 A EP 01400894A EP 01400894 A EP01400894 A EP 01400894A EP 1146732 A1 EP1146732 A1 EP 1146732A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- integrator
- input
- pel
- bus
- impedance matching
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000006243 chemical reaction Methods 0.000 title claims abstract description 48
- 239000011159 matrix material Substances 0.000 claims abstract description 11
- 230000006978 adaptation Effects 0.000 claims abstract description 10
- PXFBZOLANLWPMH-UHFFFAOYSA-N 16-Epiaffinine Natural products C1C(C2=CC=CC=C2N2)=C2C(=O)CC2C(=CC)CN(C)C1C2CO PXFBZOLANLWPMH-UHFFFAOYSA-N 0.000 claims abstract description 4
- LFQCEHFDDXELDD-UHFFFAOYSA-N tetramethyl orthosilicate Chemical compound CO[Si](OC)(OC)OC LFQCEHFDDXELDD-UHFFFAOYSA-N 0.000 claims description 18
- 210000001783 ELP Anatomy 0.000 description 23
- 230000006870 function Effects 0.000 description 17
- 230000004044 response Effects 0.000 description 15
- 238000010586 diagram Methods 0.000 description 10
- 238000012545 processing Methods 0.000 description 6
- 239000003990 capacitor Substances 0.000 description 4
- 238000003384 imaging method Methods 0.000 description 4
- 230000009467 reduction Effects 0.000 description 4
- 230000003595 spectral effect Effects 0.000 description 4
- 238000012546 transfer Methods 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000003247 decreasing effect Effects 0.000 description 3
- 230000010354 integration Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 230000002441 reversible effect Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000005670 electromagnetic radiation Effects 0.000 description 2
- 235000021183 entrée Nutrition 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 230000007704 transition Effects 0.000 description 2
- 229910000661 Mercury cadmium telluride Inorganic materials 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 230000002596 correlated effect Effects 0.000 description 1
- 230000007123 defense Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 230000036039 immunity Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000012905 input function Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 239000011325 microbead Substances 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 244000045947 parasite Species 0.000 description 1
- 230000003071 parasitic effect Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 238000004088 simulation Methods 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N25/00—Circuitry of solid-state image sensors [SSIS]; Control thereof
- H04N25/70—SSIS architectures; Circuits associated therewith
- H04N25/76—Addressed sensors, e.g. MOS or CMOS sensors
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N25/00—Circuitry of solid-state image sensors [SSIS]; Control thereof
- H04N25/60—Noise processing, e.g. detecting, correcting, reducing or removing noise
Definitions
- image sensors There are currently several types of image sensors to convert electromagnetic radiation into electrical signals. Generally, image sensors have photodetectors that transform radiation electromagnetic in photosignals. These last are then transformed into electrical signals by means an integrated reading circuit (also called CIL), which includes analog and / or digital functions.
- CIL integrated reading circuit
- the photodetectors can be carried out within the integrated reading circuit; this is the case, in particular, when the photodetectors are produced by photodiodes or photogrids of transistors CMOS operating in the visible spectral band. That case is described in particular in the article entitled “Comparison of passive and active pixel schemmes for CMOS visible imagers ”from KOZLOWSKI, KLEINHANS and LIU, SPIE conference on infrared readout electronics IV, Orlando, Florida, April 1998.
- Each ELP in the MP matrix provides, on the one hand, the coupling of the photodetector and, on the other hand, a first conversion of the photosignal into a quantity electric (current, charge or voltage).
- each row of ELPs is connected at its end to processing means deported, referenced T.
- This output fixture consists of a multiplexer M, generally of the type analog, which receives signals from each remote processing means and provides multiplexing of these signals. If the integrated CIL reading circuit has multiple PEL matrices, so the one or more multiplexer (s) M ensures (s) the multiplexing of outputs of all PEL matrices.
- the multiplexer (s) is (are) itself (themselves) connected to one or more output amplifier (s) A.
- the means of remote processing can be made from an integrator, i.e. an amplifier counter-reacted by a capacitor and a switch, which ensures the conversion into photosignal voltage delivered by the ELP either as a current or as a charge electric.
- an integrator i.e. an amplifier counter-reacted by a capacitor and a switch, which ensures the conversion into photosignal voltage delivered by the ELP either as a current or as a charge electric.
- the capacity brought back to the input of the integrator I, during the reading phase of each PEL, is then equal to the sum of the output capacity of the addressed PEL (denoted P1), of the output capacities of the unaddressed PELs. (denoted P2) and the capacity of the C x-bus connection used to ensure electrical continuity between the outputs of all the PELs and the input of the integrator I.
- the output capacity of an addressed PEL corresponds to the capacity of the addressing switch in the closed state
- the output capacity of an unaddressed PEL corresponds to the capacity of the addressing switch in the open state.
- Vref is the voltage of reference of the DC voltage source, connected on the input e + of an amplifier A; e- is the entrance negative of amplifier A to which is connected the PEL bus (referenced Bpel); Cconv is the ability to conversion connected between the output s of amplifier A and the input e- of this amplifier; and Cbus_pel is the capacity of the PEL bus.
- This expression shows the relationships between contributors to conversion noise and the sensitivity of conversion noise to these contributors.
- the voltage response obtained at the output of the remote integrator. This is the case, for example, when we want to use a capacity of low value conversion to convert to voltage, optimally, a low-value photocharge, or when you want to integrate a photocurrent for a short time, or when you want integrate a low input current. It is also the case, when we want to reduce the requirements on the input noise from analog blocks located downstream deported integrator or increase immunity noise from the CIL output signal or reduce the complexity of the signal acquisition chains output, etc. In all these cases, the voltage response can be increased by decreasing the capacity of the conversion capacitor, but this induces, according to the explanations given above, an increase conversion noise.
- the formula giving the spectral density V bs-conv shows that the noise of the reference voltage is amplified by an increasing function of the ratio Cbus_pel / Cconv.
- Obtaining a low conversion noise transfers strong constraints on the production of the power supply when the Cbus_pel / Cconv ratio is unfavorable.
- its “routing” must be subject to special precautions if one wishes to guarantee this noise level on the input e + of all the remote integrators of the integrated circuit of reading.
- the object of the invention is to remedy the disadvantages of image sensors with integrators deportees, described above. To this end, she offers a device for converting a photosignal into voltage, usable in image sensors remote integrators and presenting a noise of reduced conversion.
- the conversion noise can be reduced if you reduce significant the capacity brought back on the entry of the remote integrator, without altering the function of transfer of photosignal in tension. This is achieved by inserting, between the end of the PEL bus (used to multiplex the outputs of the elementary points of a same row) and the integrator input, a low capacity impedance matching device Release.
- the invention relates a matrix read image sensor comprising an array of connected elementary photodetectors by at least one PEL bus to a remote integrator converting the signal from each photodetector elementary in tension, characterized in that it between the end of the PEL bus and the entrance to the integrator, an impedance matching device to low output capacity, delivering at its output, during the conversion time of a signal from photodetector, a charge variation which corresponds to an affine function (i.e. a variation monotonic of the input function) of the load present at the entrance of said adaptation device.
- an affine function i.e. a variation monotonic of the input function
- the load variation can be determined by: where Iinj is the instantaneous current of the bus injected at the input of the adaptation device, Iint is the instantaneous current at the output of the adaptation device and Tconv is the conversion time.
- the adaptation device impedance is connected as close as possible to the input of the integrator.
- the adaptation device impedance is a gate-mounted TMOS transistor common on the input of the integrator.
- the impedance matching device has a common gate TMOS transistor associated with a feedback amplifier.
- the impedance matching device has two transistors and two mirrored voltage sources current.
- the invention relates to an image sensor with remote integrator, in which the conversion noise is reduced.
- This reduction in conversion noise is obtained by inserting, between the end of the PEL bus and the input of the remote integrator, a device impedance matching of low output capacity, which significantly reduces the capacity brought to the input of the remote integrator, without altering the photosignal transfer function by voltage.
- the invention therefore proposes to select a impedance matching device which respects the conservation of the charge between its entry and exit so as not to alter the conversion process, by voltage, photosignal delivered by the ELP.
- any adaptation device impedance can be used as soon as it has a low output capacity, and that it delivers, on its electrical output node, for a time Tconv equal to the duration of the conversion from photosignal to voltage, a charge variation strictly equal to the one developed on its input node.
- This charge variation is an affine function of the charge variation injected at its input; it is given by the expression: where Iint (t) is the instantaneous current at the input of the integrator.
- FIG 4 there is shown schematically the integrated circuit for reading a image sensor with remote integrator, according to the invention.
- the elementary points have been referenced P and the bus PEL connecting each row of elementary points P is referenced Bpel.
- This Bpel bus is connected to one of its ends (hereinafter called "end"), at an impedance matching device D, itself connected to the input of an integrator I.
- the integrator I can be the same as that used in the prior art and shown in the figure 3.
- the impedance matching device D can be carried out according to several embodiments different.
- the impedance matching device is made by a TMOS transistor mounted in common gate on the integrator. This embodiment is shown in Figure 5.
- the TMOS transistor T is referenced T with its gate g T , its source s T , and its drain d T.
- the source s T of transistor T is connected to the end of the PEL bus;
- the drain d T of the transitor T is connected to the input e- of the amplifier A, in other words, to the input of the integrator I;
- the gate g T of the transistor T is connected to a voltage source Vg.
- the transistor T can be an NMOS transistor, especially if we want integrate the photocurrent delivered by photodiodes of type N on a substrate P or even of a resistive microbolometer.
- the transistor T can be of the PMOS type in order to process the photocurrent delivered by P-type photodiodes on an N substrate or even a microbolometer resistive.
- Amplifier A shown in this Figure 5, has a differential input (e-; e +); however, the invention can be used with other types of charge amplifier.
- the quiescent point of transistor T is adjusted so that it delivers, at the input of amplifier A, that is to say on its drain d T , a current equal to the current Iinj injected into its source s T , by bus Bpel.
- the potential of the drain d T of the transistor is equal to Vref, which is the virtual mass of the differential amplifier A.
- the voltage applied to the gate of the transistor T is adjusted so that the transistor is in saturation mode.
- the transistor T thus has a very high drain-source resistance; moreover, its drain current d T is then equal to the current injected into the source s T of the transistor.
- the output capacity of the transistor T is equal to the sum of the capacitance gate-drain of a TMOS transistor, in saturation and the capacity of its drain junction. This capacity is of the order of magnitude of the output capacity of a single PEL. So she is very less than the capacity of the PEL bus.
- the voltages Vg and Vref are optimized, in order to ensure a functioning in regime of saturation throughout the current entry excursion, because the potential of the PEL bus must be able to vary, so that the transistor T can develop a voltage source grid compatible with current intensity injected. In this way, the voltage response of the integrator I, associated with the adaptation device impedance D, has a constant current attack on the bus ELP identical to that of a remote integrator classic.
- the curve Id T -s T shows the drain-source current of the transistor T; the values Iinj-max and Iinj-min are, respectively, the maximum and minimum values of the current injected on the source s T of transistor T, and the value V T represents the threshold voltage of transistor T.
- the ELPs of a sensor deliver photosignals whose levels vary independently of each others because the pixels of the image to which they are associates are generally not correlated. It is necessary therefore that, in the device of the invention, the response from the integrator to an amplitude current pulse and of variable duration is identical to that of a classic remote integrator. To show that is the case we have shown in figure 7 different responses from the integrator.
- Part A of FIG. 7 shows the response of the integrator to the injection of a current step Iinj (I1, I2) on the bus PEL.
- Part B of Figure 7 shows that we obtain, either by solving the KIRCHOFF equations, or by performing appropriate electrical simulations, that the current Iint injected into the integrator follows the variation of the current Iinj with a response time finished.
- Part C of FIG. 7 shows the temporal evolution of the potential of the bus PEL between these two asymptotic values V1 and V2 which are determined by means of the current-voltage characteristic of FIG. 6.
- the time constant ⁇ which governs this transient regime, is given by the formula: ⁇ ⁇ gm / Cbus_pel, where gm is the transductance of transistor T.
- the device the invention does not allow delivery at all times t an output current equal to its input current, it retains the charge between its entry and exit, from when the conversion time is greater than the time response of the device and that the induced variation on the PEL bus by the current pulse delivered by each ELP does not pass the junctions which it has connected in reverse.
- the output capacity of this device is very lower than that of the PEL bus, of an integrated circuit of read in a matrix sensor.
- the adaptation device impedance achieved by a mounted TMOS transistor in common grid therefore meets the characteristics previously stated and necessary for a good operation of an image sensor, namely a low output capacity and delivery on its output node of a load variation strictly equal to that developed at the place of entry.
- the order of magnitude of Cbus_pel is 2.0 pF and that of Cconv is approximately 0.1 pF.
- the capacity C less can be reduced to 0.1 pF.
- the invention therefore makes it possible to reduce significantly the conversion noise in the white noise.
- the impedance matching device can be produced according to other embodiments.
- it can be achieved by means of a TMOS transistor with a common gate, with a feedback amplifier.
- a feedback amplifier it is possible to further improve certain characteristics of the first embodiment by counter-reacting the source of the transistor T with an amplifier G.
- the amplifier G is mounted between the gate g T of the transistor T and the source s T of transistor T, as shown in Figure 8.
- the introduction of this feedback has the effect of increasing the input transconductance of transistor T, which results in a reduction of the response time to one step current.
- Such a device can be used, for example example, in integrated reading circuits where the conversion time requirements (i.e. reading time of the information delivered on an ELP) and the voltage response of the remote integrator require reducing the response time of the impedance matching device D located upstream of the integrator.
- the conversion time requirements i.e. reading time of the information delivered on an ELP
- the voltage response of the remote integrator require reducing the response time of the impedance matching device D located upstream of the integrator.
- the impedance matching device can also be realized by means of a current mirror, as shown in figure 9.
- the impedance matching device D is produced by means of two transistors T1 and T2, each associated with a voltage source V1 and V2 and connected to each other by their gate g T so as to produce a current mirror.
- the device of the invention delivers at output a current Iint which is equal to its input current Iinj multiplied by an amplification factor which is a function of the geometry ratio of the TMOS transistors T1 and T2 and of the voltages V1 and V2 .
- the current gain may be less than or greater than unity.
- the device of the invention produced according to this embodiment can be used in applications where it is necessary to crop the current delivered by the PEL bus in the excursion charge amplifier input.
- the image sensor of the invention allows therefore to obtain a conversion noise lower than that of a classic sensor.
- the dynamics of inflow of the sensor is thus increased, the noise reduced to the input of the integrated reading circuit being decreased.
- the device of the invention allows, more, to get a better voltage response to the remote integrator output, reducing the converting capacity and decreasing noise by conversion.
- CIL CIL-in-dielectric-in-dielectric-in-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dielectric-dos, thermosensors, including microbolometers resistive to bashing in remote current.
- devices impedance matching according to the invention can also be associated with deported integrators multi-fiber (charge amplifiers with several capacitors selectable in its loop feedback), in order to convert adapted to the level of the input photosignal.
- deported integrators multi-fiber charge amplifiers with several capacitors selectable in its loop feedback
- the device of the invention can accommodate a level noise on the reference voltage Vref greater than that of a classic integrator. In these same conditions it can also accommodate a level charge amplifier input noise higher than that of a traditional remote integrator.
- the conversion noise is no longer a function the capacity of the PEL bus. It is therefore possible increase this capacity without increasing the noise of conversion. This opens up many possibilities, such as increasing the format of the sensor, increasing the pace of the ELP, the possibility increase the number of multiplexed rows towards a same integrator, increasing the complexity of the PEL or the increase in the number of entries and out of the ELP.
Landscapes
- Engineering & Computer Science (AREA)
- Multimedia (AREA)
- Signal Processing (AREA)
- Solid State Image Pick-Up Elements (AREA)
- Amplifiers (AREA)
- Transforming Light Signals Into Electric Signals (AREA)
- Light Receiving Elements (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR0004562 | 2000-04-10 | ||
FR0004562A FR2807601B1 (fr) | 2000-04-10 | 2000-04-10 | Dispositif de conversion d'un photosignal en tension dans les senseurs d'images a integrateurs deportes |
Publications (2)
Publication Number | Publication Date |
---|---|
EP1146732A1 true EP1146732A1 (de) | 2001-10-17 |
EP1146732B1 EP1146732B1 (de) | 2009-10-21 |
Family
ID=8849071
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP01400894A Expired - Lifetime EP1146732B1 (de) | 2000-04-10 | 2001-04-06 | Photosignal-Spannungswandlerschaltung in Bildsensoren mit entfernten Integratoren |
Country Status (4)
Country | Link |
---|---|
US (1) | US7060956B2 (de) |
EP (1) | EP1146732B1 (de) |
DE (1) | DE60140230D1 (de) |
FR (1) | FR2807601B1 (de) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2031452B1 (de) * | 2007-08-27 | 2017-10-11 | Xeikon Manufacturing | Zweikomponenten-Toner mit zwei Walzen |
KR101513373B1 (ko) * | 2013-12-31 | 2015-04-20 | 한양대학교 산학협력단 | 직류 오프셋을 보상하는 광통신 수신기 |
US10448053B2 (en) * | 2016-02-15 | 2019-10-15 | Qualcomm Incorporated | Multi-pass non-separable transforms for video coding |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62149256A (ja) * | 1985-09-19 | 1987-07-03 | Seiko Epson Corp | イメ−ジセンサ信号読出回路 |
JPS62292081A (ja) * | 1986-06-12 | 1987-12-18 | Seiko Epson Corp | イメ−ジセンサ信号続出回路 |
FR2736782A1 (fr) * | 1995-04-07 | 1997-01-17 | Commissariat Energie Atomique | Dispositif et procede de lecture d'une matrice de detecteurs photoniques |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2735632B1 (fr) * | 1995-06-14 | 1997-07-11 | Commissariat Energie Atomique | Dispositif et procede de numerisation pour detecteurs photosensibles et procede de lecture d'une matrice de detecteurs photoniques |
-
2000
- 2000-04-10 FR FR0004562A patent/FR2807601B1/fr not_active Expired - Fee Related
-
2001
- 2001-04-05 US US09/826,040 patent/US7060956B2/en not_active Expired - Fee Related
- 2001-04-06 EP EP01400894A patent/EP1146732B1/de not_active Expired - Lifetime
- 2001-04-06 DE DE60140230T patent/DE60140230D1/de not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62149256A (ja) * | 1985-09-19 | 1987-07-03 | Seiko Epson Corp | イメ−ジセンサ信号読出回路 |
JPS62292081A (ja) * | 1986-06-12 | 1987-12-18 | Seiko Epson Corp | イメ−ジセンサ信号続出回路 |
FR2736782A1 (fr) * | 1995-04-07 | 1997-01-17 | Commissariat Energie Atomique | Dispositif et procede de lecture d'une matrice de detecteurs photoniques |
Non-Patent Citations (3)
Title |
---|
PATENT ABSTRACT OF JAPAN, vol. 012, no. 189, 2 June 1988 (1988-06-02), pages E-616 |
PATENT ABSTRACTS OF JAPAN vol. 011, no. 384 (E - 565) 15 December 1987 (1987-12-15) * |
PATENT ABSTRACTS OF JAPAN vol. 012, no. 189 (E - 616) 2 June 1988 (1988-06-02) * |
Also Published As
Publication number | Publication date |
---|---|
DE60140230D1 (de) | 2009-12-03 |
US20010048065A1 (en) | 2001-12-06 |
US7060956B2 (en) | 2006-06-13 |
EP1146732B1 (de) | 2009-10-21 |
FR2807601A1 (fr) | 2001-10-12 |
FR2807601B1 (fr) | 2002-09-20 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0749233B1 (de) | Digitalisierungsvorrichtung und -verfahren für lichtempfindliche Detektoren und Ausleseverfahren einer Matrix von Lichtdetektoren | |
JP4310428B2 (ja) | 光検出器の単光子読出し用のコンパクトな超低雑音広帯域幅ピクセル増幅器 | |
FR2825219A1 (fr) | Pixel actif cmos a bruit reduit | |
EP1354360B1 (de) | Photoelektrisches element mit sehr grossem dynamikbereich | |
EP2143264B1 (de) | Laserimpulsmatrixdetektor mit schneller summierung | |
EP0883900B1 (de) | Vorrichtung und ausleseverfahren einer matrix von lichtdetektoren | |
EP1146732B1 (de) | Photosignal-Spannungswandlerschaltung in Bildsensoren mit entfernten Integratoren | |
EP0692907B1 (de) | Schaltung zur Unterdrückung des Dunkelstromes eines Photodetektors | |
EP1361613B1 (de) | Fotoempfangende Vorrichtung, Laserimpulsdetektor mit einer solchen Vorrichtung und Laserimpulsdetektorvorrichtung mit solchen Laserimpulsdetektoren | |
EP0182679B1 (de) | Photoempfindliche Zwischenspaltanordnung mit zurückgekoppeltem Verstärker | |
EP1367817A1 (de) | Aktiver CMOS-Pixel mit verringertem Geräusch | |
FR3046679A1 (fr) | Circuit de detection de rayons x pour capteur radiologique dentaire | |
EP0354106B1 (de) | Rauscheliminierende Schaltung, die in einer Festkörperbildaufnahmevorrichtung integriert ist | |
FR2736782A1 (fr) | Dispositif et procede de lecture d'une matrice de detecteurs photoniques | |
FR2759509A1 (fr) | Circuit integrateur a linearite amelioree | |
EP0654945B1 (de) | Ladungseinspritzschaltung zur thermischen Abbildung | |
EP1346231B1 (de) | Verfahren und geräte zur analogen verarbeitung eines von einem teilchendetektor emittierten signals | |
FR2638309A1 (fr) | Plaquette de pretraitement des courants de sortie de diodes de detection soumises a un rayonnement thermique | |
EP3829160B1 (de) | Pixel mit einstellbarem dynamikbereich zur geräuschreduzierung | |
EP0848547B1 (de) | Schnittstellenschaltung für Videokamera | |
FR3111014A1 (fr) | Capteur d’image matriciel à sensibilité élevée | |
FR2859345A1 (fr) | Detecteur de rayonnements a grande dynamique | |
FR2609843A1 (fr) | Dephaseur actif 0-180o pour hyperfrequences | |
WO1999035820A1 (fr) | Dispositif de prise de vue a transfert de charges sur un element de connexion | |
EP1215890A1 (de) | Ladungsleseschaltung und -verfahren auf der Basis einer Kalibrierung |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): AT BE CH CY DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE TR Kind code of ref document: A1 Designated state(s): DE GB IT |
|
AX | Request for extension of the european patent |
Free format text: AL;LT;LV;MK;RO;SI |
|
17P | Request for examination filed |
Effective date: 20020322 |
|
AKX | Designation fees paid |
Free format text: DE GB IT |
|
RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: COMMISSARIAT A L'ENERGIE ATOMIQUE |
|
17Q | First examination report despatched |
Effective date: 20080428 |
|
GRAP | Despatch of communication of intention to grant a patent |
Free format text: ORIGINAL CODE: EPIDOSNIGR1 |
|
GRAS | Grant fee paid |
Free format text: ORIGINAL CODE: EPIDOSNIGR3 |
|
GRAA | (expected) grant |
Free format text: ORIGINAL CODE: 0009210 |
|
AK | Designated contracting states |
Kind code of ref document: B1 Designated state(s): DE GB IT |
|
REG | Reference to a national code |
Ref country code: GB Ref legal event code: FG4D Free format text: NOT ENGLISH |
|
REF | Corresponds to: |
Ref document number: 60140230 Country of ref document: DE Date of ref document: 20091203 Kind code of ref document: P |
|
PLBE | No opposition filed within time limit |
Free format text: ORIGINAL CODE: 0009261 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: NO OPPOSITION FILED WITHIN TIME LIMIT |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: DE Payment date: 20100423 Year of fee payment: 10 Ref country code: IT Payment date: 20100423 Year of fee payment: 10 |
|
26N | No opposition filed |
Effective date: 20100722 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: GB Payment date: 20100420 Year of fee payment: 10 |
|
REG | Reference to a national code |
Ref country code: DE Ref legal event code: R119 Ref document number: 60140230 Country of ref document: DE |
|
REG | Reference to a national code |
Ref country code: DE Ref legal event code: R119 Ref document number: 60140230 Country of ref document: DE |
|
GBPC | Gb: european patent ceased through non-payment of renewal fee |
Effective date: 20110406 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: IT Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20110406 Ref country code: GB Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20110406 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: DE Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 20111031 |